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This paper presents a novel framework for simulating quantum spin dynamics by utilizing a variational product-state ansatz that deliberately excludes intersite entanglement while retaining local quantum effects. By deriving nonlinear dynamics from mean-field interdependence and state-dependent dissipation, the authors establish an efficient O(N) method to bridge classical atomistic models with the quantum regime for arbitrary spins. This approach offers significant practical value for modeling materials where entanglement remains negligible, clarifying the geometric origins of differences between quantum and classical Landau-Lifshitz dynamics.
Nonlinear quantum multi-spin dynamics without entanglement
arXiv:2610.05521v1 Announce Type: new Abstract: We introduce a distinct route for extending classical atomistic spin dynamics into the quantum regime for arbitrary spin $s$, based on a variational product-state \textit{ansatz} that includes both pure and mixed local states. By construction, intersite entanglement -- expected to remain negligible even on very short time scales in many real materials -- is excluded, while local quantum effects are retained through the nonclassical structure of $s\geq 1$ density operators, and nonlinear dynamics arise from both the mean-field interdependence of the local states and the state-dependent dissipative terms. This framework clarifies the variational and geometric origin of the inequivalence between quantum Landau-Lifshitz and Landau-Lifshitz-Gilbert dynamics, provides a criterion for their equivalence under a common time rescaling, establishes connections with the classical theory through two qualitatively distinct limits ($s\to\infty$ and a large number of quantum spins $N$), and allows realistic $\mathcal{O}(N)$ simulations of quantum spin dynamics in materials.
Abstract:We introduce a distinct route for extending classical atomistic spin dynamics into the quantum regime for arbitrary spin $s$, based on a variational product-state \textit{ansatz} that includes both pure and mixed local states. By construction, intersite entanglement -- expected to remain negligible even on very short time scales in many real materials -- is excluded, while local quantum effects are retained through the nonclassical structure of $s\geq 1$ density operators, and nonlinear dynamics arise from both the mean-field interdependence of the local states and the state-dependent dissipative terms. This framework clarifies the variational and geometric origin of the inequivalence between quantum Landau-Lifshitz and Landau-Lifshitz-Gilbert dynamics, provides a criterion for their equivalence under a common time rescaling, establishes connections with the classical theory through two qualitatively distinct limits ($s\to\infty$ and a large number of quantum spins $N$), and allows realistic $\mathcal{O}(N)$ simulations of quantum spin dynamics in materials.
Quantum Physics (quant-ph); Mesoscale and Nanoscale Physics (cond-mat.mes-hall); Strongly Correlated Electrons (cond-mat.str-el)
arXiv:2610.05521 [quant-ph]
(or arXiv:2610.05521v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2610.05521 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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